Convert units: nm, mm and cm to m, and check whether angles are measured from the normal.
Check signs and plausibility: a virtual image has dᵢ < 0, an approaching source sounds higher, a closed pipe has only odd harmonics.
2Practice problems
1.KinematicsMedium
A car speeding at a constant 33 m/s passes a police car standing still. At that moment the police car starts and accelerates uniformly at 6 m/s². How far from its starting point does the police car catch up? Find d.
vcar = 33 m/sapolice = 6 m/s²v0,police = 0
d = m
2.KinematicsHard
Ball A is dropped from rest from a height of 25 m. At the same instant ball B is thrown straight up from the ground directly below at 23 m/s. Ignore air resistance and use g = 9.81 m/s². When do the balls meet? Find t.
H = 25 mv0B = 23 m/sg = 9.81 m/s²
t = s
3.Newton’s lawsMedium
A 40 kg sled is pulled across level snow by a rope at 15° above the horizontal with a force of 180 N. The coefficient of kinetic friction is 0.1. Use g = 9.81 m/s². Find the acceleration a of the sled.
m = 40 kgF = 180 Nθ = 15°μ = 0.1g = 9.81 m/s²
a = m/s²
4.Newton’s lawsHard
An 8.5 kg block on a ramp at 35° is connected by a light string over a frictionless pulley at the top of the ramp to a hanging 9 kg mass. The hanging mass moves down. The coefficient of kinetic friction between block and ramp is 0.1. Use g = 9.81 m/s². Find the acceleration a of the system.
m1 = 8.5 kgm2 = 9 kgθ = 35°μ = 0.1g = 9.81 m/s²
a = m/s²
5.Projectile motionMedium
A ball is launched from level ground at 55° above the horizontal and lands 55 m away. Ignore air resistance and use g = 9.81 m/s². Find the launch speed v0.
θ = 55°R = 55 mg = 9.81 m/s²
v0 = m/s
6.Projectile motionHard
A ball is launched at 33 m/s and 60° above the horizontal from the top of a 10 m cliff. Ignore air resistance and use g = 9.81 m/s². At what angle α below the horizontal does it hit the ground?
v₀ = 33 m/sθ = 60°h = 10 mg = 9.81 m/s²
α = °
7.Work & energyMedium
A 2.5 kg block slides 20 m down a slope at 25° to the horizontal, with a coefficient of kinetic friction of 0.3. Find the work Wf done against friction.
m = 2.5 kgθ = 25°μ = 0.3d = 20 mg = 9.81 m/s²
Wf = J
8.Work & energyHard
A 5 kg block starts from rest at the bottom of a 20° slope and is pulled up the slope by a constant force of 40 N parallel to the slope. The coefficient of kinetic friction is 0.25. Find the speed v of the block after it has moved 2 m up the slope.
A 1400 kg car moving at 13 m/s runs into a stationary 800 kg car and the two lock together. What percentage ΔK/K of the original kinetic energy is lost?
m1 = 1400 kgv1 = 13 m/sm2 = 800 kgv2 = 0
ΔK/K = %
10.Momentum & collisionsHard
At a crossing an 800 kg car travelling east at 17 m/s collides with a 1600 kg car travelling north at 17 m/s. The cars lock together. Find the direction θ of the wreck just after the collision, measured north of east.
m1 = 800 kgv1 = 17 m/s (E)m2 = 1600 kgv2 = 17 m/s (N)
θ = °
11.Hydrostatic forceMedium
A vertical rectangular gate 1.5 m wide sits in the wall of a tank of water, with its top edge 2.5 m below the surface. Find the resultant hydrostatic force F on the gate.
A vertical rectangular gate 2 m wide sits in the wall of a tank of glycerin, with its top edge 0.5 m below the surface. Find the depth ycp of the centre of pressure below the surface.
Water flows through a horizontal pipe that narrows from 100 mm to 75 mm. In the wide section the pressure is 120 kPa and the velocity is 1 m/s. Ignoring losses, find the pressure p2 in the narrow section.
Water flows up through a pipe that narrows from 75 mm to 50 mm while rising 10 m. At section 1 the pressure is 240 kPa and the velocity is 2.5 m/s. Ignoring losses, find the pressure p2 at section 2.
A heat engine works between a hot reservoir at 350 °C and a cold reservoir at 30 °C. It takes in 3100 kJ of heat. Find the most work Wmax it could possibly produce.
TH = 350 °CTL = 30 °CQH = 3100 kJ
Wmax = kJ
18.Heat engines & refrigeratorsHard
A heat engine takes in 1200 kJ of heat from a reservoir at 600 °C, produces 396 kJ of work and rejects the rest to a reservoir at 25 °C, per cycle. Find the total entropy generated Sgen per cycle.
TH = 600 °CTL = 25 °CQH = 1200 kJW = 396 kJ
Sgen = kJ/K
19.Waves, sound & opticsMedium
A pipe closed at one end must have its harmonic number 3 at 643 Hz. The speed of sound is 343 m/s. Find the length L of the pipe.
v = 343 m/sn = 3f3 = 643 Hz
L = m
20.Waves, sound & opticsHard
Light of wavelength 589 nm falls at right angles on a grating with 200 lines per millimetre. Find the angle θ2 of the order-2 maximum.
N = 200 mm⁻¹λ = 589 nmm = 2
θ2 = °
3Solutions
1.Kinematics
Answer: d = 363 m
Motion with constant acceleration: v = v₀ + a·t, s = v₀·t + ½·a·t² and v² = v₀² + 2·a·s. Pick the equation that contains the three things you know and the one you want, and keep the signs consistent with one positive direction.
Equal distances
v·t = ½·a·t² → t = 2v/a = 2·33/6 = 11 s
Distance
d = v·t = 33·11 = 363 m
Answer
d = 363 m
At that moment the police car moves at 2v = 66 m/s.
2.Kinematics
Answer: t = 1.087 s
Motion with constant acceleration: v = v₀ + a·t, s = v₀·t + ½·a·t² and v² = v₀² + 2·a·s. Pick the equation that contains the three things you know and the one you want, and keep the signs consistent with one positive direction.
Meeting time
Up is positive, the ground is y = 0.
25 − ½g·t² = 23·t − ½g·t² → t = 25/23 = 1.087 s
Answer
t = 1.087 s
3.Newton’s laws
Answer: a = 3.482 m/s²
Newton’s second law: the net force on a body equals its mass times its acceleration, ΣF = m·a. Draw a free-body diagram, choose a positive direction along the motion, and add every force in that direction: applied forces, friction μ·N against the motion, and the components of gravity.
Normal force
N = m·g − F·sin θ = 392.4 − 180·sin 15° = 345.8 N
Horizontal forces
m·a = F·cos θ − μ·N = 173.9 − 34.58
a = 139.3/40 = 3.482 m/s²
Answer
a = 3.482 m/s²
4.Newton’s laws
Answer: a = 1.922 m/s²
Newton’s second law: the net force on a body equals its mass times its acceleration, ΣF = m·a. Draw a free-body diagram, choose a positive direction along the motion, and add every force in that direction: applied forces, friction μ·N against the motion, and the components of gravity.
Forces along the string
m₂·g = 88.29 N
m₁·g·sin θ = 47.83 N
μ·m₁·g·cos θ = 6.83 N
Acceleration of the system
a = (88.29 − 47.83 − 6.83)/17.5 = 1.922 m/s²
Answer
a = 1.922 m/s²
5.Projectile motion
Answer: v0 = 23.96 m/s
Projectile motion: with no air resistance, x = vxt and y = h + vyt − ½gt². The two directions are independent except that they share the same time.
Solve the range formula for v₀
v₀ = √(g·R/sin 2θ) = √(9.81·55/sin 110°) = 23.96 m/s
Answer
v0 = 23.96 m/s
6.Projectile motion
Answer: α = 62.6 °
Projectile motion: with no air resistance, x = vxt and y = h + vyt − ½gt². The two directions are independent except that they share the same time.
Split the launch velocity
vx = 33·cos 60° = 16.5 m/s
vy0 = 33·sin 60° = 28.58 m/s
Vertical speed at impact
Energy or v² = v₀² + 2as in the vertical direction.
vy = √(28.58² + 2·9.81·10) = 31.83 m/s
Impact angle
tan α = vy/vx = 31.83/16.5 → α = 62.6°
Answer
α = 62.6°
7.Work & energy
Answer: Wf = 133.4 J
Work–energy principle: the change in kinetic energy equals the work done by all forces. Writing gravity and springs as potential energy (mgh and ½kx²) turns this into a balance: initial energy = final energy + energy lost to friction (μN·d).
Friction force
N = mg·cos θ = 24.53·0.9063 = 22.23 N
F = μN = 0.3·22.23 = 6.668 N
Work against friction
Wf = F·d = 6.668·20 = 133.4 J
Answer
Wf = 133.4 J
8.Work & energy
Answer: v = 3.06 m/s
Work–energy principle: the change in kinetic energy equals the work done by all forces. Writing gravity and springs as potential energy (mgh and ½kx²) turns this into a balance: initial energy = final energy + energy lost to friction (μN·d).
Forces along the slope
m·g = 5·9.81 = 49.05 N
mg·sin θ = 16.78 N
μ·mg·cos θ = 11.52 N
Work–energy
½mv² = (40 − 28.3)·2 = 23.4 J
v = √(2·23.4/5) = 3.06 m/s
Answer
v = 3.06 m/s
9.Momentum & collisions
Answer: ΔK/K = 36.36 %
Conservation of momentum: when no external force acts during a collision, the total momentum Σm·v before equals the total after. Velocities have a direction, so pick a positive direction and give velocities the other way a minus sign. In an elastic collision kinetic energy is conserved too; in a perfectly inelastic one the bodies stick together.
Common velocity
v′ = m1·v1/(m1 + m2) = 1400·13/2200 = 8.273 m/s
Kinetic energy before and after
Kbefore = ½·1400·13² = 118300 J
Kafter = ½·2200·8.273² = 75282 J
Fraction lost
ΔK/K = 43018/118300 = 36.36 %
Answer
ΔK/K = 36.36 %
The lost energy goes into deformation, heat and sound.
10.Momentum & collisions
Answer: θ = 63.43 °
Conservation of momentum: when no external force acts during a collision, the total momentum Σm·v before equals the total after. Velocities have a direction, so pick a positive direction and give velocities the other way a minus sign. In an elastic collision kinetic energy is conserved too; in a perfectly inelastic one the bodies stick together.
Momentum components
px = 800·17 = 13600 kg·m/s
py = 1600·17 = 27200 kg·m/s
Direction
tan θ = py/px = 2 → θ = 63.43°
Answer
θ = 63.43°
11.Hydrostatic force
Answer: F = 44.15 kN
Hydrostatic force on a plane surface: F = ρ·g·yc·A. It acts at the centre of pressure, ycp = yc + Ic/(ycA), which always lies below the centroid.
Centroid depth and area
yc = d + H/2 = 2.5 + 1/2 = 3 m
A = H·b = 1·1.5 = 1.5 m²
Resultant force
F = ρ·g·yc·A = 1000·9.81·3·1.5 = 44.15 kN
Answer
F = 44.15 kN
12.Hydrostatic force
Answer: ycp = 1.4 m
Hydrostatic force on a plane surface: F = ρ·g·yc·A. It acts at the centre of pressure, ycp = yc + Ic/(ycA), which always lies below the centroid.
Centroid depth and area
yc = d + H/2 = 0.5 + 1.5/2 = 1.25 m
A = H·b = 1.5·2 = 3 m²
Resultant force
F = ρ·g·yc·A = 1260·9.81·1.25·3 = 46.35 kN
Centre of pressure
Pressure grows with depth, so the resultant acts below the centroid.
Continuity and Bernoulli: for an incompressible fluid the flow rate is the same at every section, Q = A₁v₁ = A₂v₂. Along a streamline without losses, p + ½ρv² + ρgz is constant, so where the fluid is faster or higher its pressure is lower.
Continuity and Bernoulli: for an incompressible fluid the flow rate is the same at every section, Q = A₁v₁ = A₂v₂. Along a streamline without losses, p + ½ρv² + ρgz is constant, so where the fluid is faster or higher its pressure is lower.
Second-law limits: no cycle working between reservoirs at absolute temperatures TH and TL can beat the reversible (Carnot) cycle: ηmax = 1 − TL/TH, COPR,max = TL/(TH − TL) and COPHP,max = TH/(TH − TL). Energy is always conserved: QH = W + QL.
Absolute temperatures
TH = 350 + 273.15 = 623.1 K
TL = 30 + 273.15 = 303.1 K
Carnot efficiency
ηmax = 1 − TL/TH = 1 − 303.1/623.1 = 51.35 %
Maximum work
Wmax = ηmax·QH = 0.5135·3100 = 1592 kJ
Answer
Wmax = 1592 kJ
18.Heat engines & refrigerators
Answer: Sgen = 1.322 kJ/K
Entropy generation: over a full cycle the working fluid has no net entropy change. The hot reservoir loses QH/TH and the cold reservoir gains QL/TL. Their sum is the entropy generated, which is zero for a reversible cycle and positive for every real one.
Heat rejected
QL = QH − W = 1200 − 396 = 804 kJ
Absolute temperatures
TH = 600 + 273.15 = 873.1 K
TL = 25 + 273.15 = 298.1 K
Entropy changes of the reservoirs
ΔSH = −1200/873.1 = −1.374 kJ/K
ΔSL = 804/298.1 = 2.697 kJ/K
Sgen = 2.697 − 1.374 = 1.322 kJ/K
Answer
Sgen = 1.322 kJ/K
Sgen > 0, so the engine is possible but irreversible.
19.Waves, sound & optics
Answer: L = 0.4001 m
Standing waves and the Doppler effect: a string fixed at both ends, or a pipe open at both ends, fits whole half-wavelengths: L = nλ/2, fn = n·v/(2L), n = 1, 2, 3, … A pipe closed at one end has a node at the closed end and an antinode at the open end: L = nλ/4 with odd n only, fn = n·v/(4L). When source or observer move along the line between them, f′ = f·(v ± vo)/(v ∓ vs): use the upper signs for motion towards each other. Two waves of nearly equal frequency beat at |f₁ − f₂|.
Wavelength
λ = v/f = 343/643 = 0.5334 m
Length
L = nλ/4 = 3·0.5334/4 = 0.4001 m
Answer
L = 0.4001 m
20.Waves, sound & optics
Answer: θ2 = 13.63 °
Interference and diffraction: light from two slits a distance d apart reaches a point on the screen with a path difference d·sin θ. Bright fringes appear where d·sin θ = mλ (m = 0, ±1, ±2, …). For a screen at distance L ≫ d, the m-th bright fringe is at y = mλL/d and the fringe spacing is Δy = λL/d. A grating with N lines per millimetre has d = 1/N and sharp maxima at d·sin θ = mλ; since sin θ ≤ 1, the highest order is the largest whole number m ≤ d/λ. A single slit of width a has dark fringes at a·sin θ = mλ, m = ±1, ±2, …